Apparatus for utilizing an expansive force.



H.-A. HUMPHREY.

APPARATUS FOR UTILIZING AN EXPANSIVE FORCE. APPLICATION FILED oc'r. 21.1911. RENEWED mm! 24. mm

1,258,570. Patented Mar. 5, 1918.

1 SHEE'I'HIIEET 1 39 38 m 20 ENTO wrnvzasss A; WM

M I BY m I I ATTORNEY H. A. HUMPHFIEY.

APPARATUS FOR UTILIZING AN EXPANSIVE FORGE- APPLICATION FILED ocr. 21.1911. nmzwsn JULY 24.1912.

1,258,570. Patented Mar. 5, 191a.

F ISHEETS-SIIEET 3.

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o as 9 5 r Y I 1s as y 2 Q10 mvsuron WITNESSES a A 4 BY a H. A. HUMPHREY. APPARATUS FOR UTILIZING AN EXPANSIVE FORCE.

APPLICATION man on. 21.1911. nzucwzo JULY 24. Ian.

1,258,570. Patented Mar. 5, 1918.

I SHEETS-SHEET 4.

ATTORNEY A 1,258,570. Patented Mar. 5, 1918.

H. A. HUMPHHEY.

APPARATUS FOR UTILIZING AN EXPANSIVE FORCE. APPLICATION HLE'D ocr. 21.1911. RENEWED JULY 24. 1911.

1 SHEETS-SHEET 5- INVENTOR WYITAVESSES W W WWM 76.; ATTORNEY H. A. HUMPHREY.

APPARATUS-FOR UTILIZING AN EXPANSIVE FORCE.

APPLICATION FILED OCT. 21. Hill. RENEWED JULY 24, I917- 1,258,570. Patented Mar. 5, 1918.

i SHEETS-SHEET 6.

7 INVENTOR mu E8 if? ATTORNEY H. A. HUMPHREY.

APPARATUS FOR unuzmam EXPANSIVE macs.

5, 191a- I SHEETS-SHEET I.

Patented INVINTOR WITNESSES ATTORNEY UNITED STATES PATENT OFFICE.

HERBERT ALFRED HUMPHREY, OF LONDON, ENGLAND, ASSIGNOR TO HUMPHREY GAS PUMP COMPANY, A CORPORATION OF NEW YORK.

APPARATUS FOR UTILIZING AN EXP ANSIVE FORCE.

Specification of Letters Patent.

Patented Mar. 5, 1918.

Original application filed June 13, 1908, Serial No. 438,425. Divided and this application filed October 21,

1911, Serial No. 655,973. Renewed July 24, 1917. Serial No. 182,585.

To all whom it may concern:

Be it known that I, HERBERT ALFRED HUMPHREY, a subject of the King of Great Britain, residing in London, England, have invented a new and useful Apparatus for Utilizing an Expansive Force, of which the following is a specification.

My invention relates to improvements in means-for utilizing an expansive force, such for example as the expansive :t'orce of an ignited combustible charge under pressure. My object is to provide an improved means whereby this expansive force may be utilined in causing the reciprocation of a body oi? liquid, the movement in one direction of said reciprocation being due to said expansive force, and utilizing the momentum of the liquid body in both directions whereby liquid is delivered to a greater head, or energy is stored, fresh liquid is entrained, the exhausted charge is expelled and a fresh expansible charge is entrained and compressed.

The invention is especially applicable to pumps or compressors.

The accompanying drawings illustrate, merely by way of example, suitable apparatus for eflecting my invention.

Figure 1 is-a vertical section of a portion of my device showing the combustion and expansion chamber and valves connected therewith, a branch adapted to connect with a source of supply and another branch adapted to connect with a play pipe leading to a reservoir or other means for storing energy, not shown.

Fig. 2 is a similar view showing a modified form of valve control.

Fig. 3 is a cross'section showing a modified form of water-valve.

Fig. a is a vertical sectional view on an enlarged scale, or the valve controlling mechanism shown in Fig. 1.

Fig. 5 is a similar view, oi? the valve controlling mechanism shown in Fig. 2.

Figs. 6 to 26 are diagrammatic views in vertical section, showing various modifica' tions of apparatus suitable for effecting my invention.

Similar numerals refer to similar parts throughout the several views.

This application is a division of my application entitled Methods of raising or forcing liquids and apparatus therefor filed June 13, 1908, Serial No. 438,d25.

The precise action of apparatus of this kind depends on the relative and absolute capacity, situation and length of the supply pipe, the delivery pipe, and the auxiliary suction pipe, when such is used, and it may be advantageous to place air chambers in one or more of these pipes.

In Fig. 1, 1 is the combustion and expansion chamber, 2 is the supply pipe communieating with a tank the level of the liquid in which is, say, at a-(. 3 is the discharge pipe the length and dimensions of which must be such that the moving mass of liquid will acquire the momentum necessary for the efiects to be produced. A valve 1 pivoted at 5 is adapted to close either the communication between chamber 1 and the supply pipe, as shown, or that between the chamber and the discharge pipe as indicated in dotted lines. At the top of the combustion chamher there are an exhaust valve 6 and a mixture inlet valve 7, the former being preferably in a plug 11 and the latter in a plug 12 in the casting 10. The discharge pipe is in communication through a non-return valve 9 with a pipe 20 connected with the aforesaid supply tank or with another supply of liquid which may be at a lower level than that tank.

Leaving for the moment the mechanism by which the valves 6 and 7 are operated, the cycle in such an apparatus is as follows:--

Assuming the position of the parts to be that shown and chamber 1 to contain liquid up to a level represented for instance by the line 6-5, above which is combustible mixture suitably compressed, ignition occurs, such as by means of the sparking plug 74, and the liquid is driven along the discharge pipe to a place of higher pressure or higher level. When the products of combustion have expanded to a certain degree, say to the level 0-0, the position of which will depend, among other factors, on the height of the surface of the liquid in the supply tank above the valve l, the pressure in the chamber tending to keep the valve 1 closed, falls below that in the pipe 2 tending to open the valve, whereupon the latter swings over to the position 1 shown in dotted lines.

Liquid now flows into the chamber from the supply tank expelling the products of combustion, through the valve 6 which has chamber commences to return the valve 7 is opened and valve 6 is closed. The liquid now returns, and in doing so draws in the fresh charge through valve 7 which then closes.

At the time when the valve 4 took up the position 4*, the liquid in the discharge pipe had attained considerable velocity, and on account of the length of the pipe the kinetic energy stored in the moving column is considerable, so that the latter continues its motion after the valve 4: has come into position 1 and draws liquid into the discharge pipe through valve 9. I

Presently thecolumn comes to rest, valve 9 closes automatically and under the action of the inwardly flowing column of liquid, valve 4 now swings overtto its original posi-- tion and the returning liquid enters the chamber and compresses the charge. The

- cycle then begins again.

The valve distribution is in this example as follows :Rigidly connected with valve 4: is an arm 21' to which is pivoted one end of a rod 22. The other end of this rod,

shown drawn to an enlarged scale in Fig.

l, extends through a sleeve 25pivoted' to an arm 26 or" a short rocking shaft 27. This,v

end of the and carries two tappets 23, 24-. When the valve 1 swings over as described above, rod 22 is pulled downward andoat a predetermined period of its stroke tappet -23 depresses the lever 26 and therefore the arm 28 which is also keyed to shaft 27. The

last named arm rests on'a pawl 34 pivoted to the end of the stem of the exhaust valve 6 and normally in line with the axis thereof; thus the depression of the arm opens the valve. Meanwhile the tappet 2 1 has turned.

an arm 29 of a short rocking shaft which also carries a pawl 17 the latter is thus disengaged from the collar 16 on-the stem of the inlet valve 7 which until now it has prevented from moving. The spring 15, however, attached at one end to the valve spindle and at the other end to a post 19, still keeps this valve shut. The products of combustion are now expelled as already described past valve 6 and a non-return valve 8 which is inserted in the exhaust pipe 13 to prevent the.

products from being sucked back again into the chamber during the return movement of in through pipe 14. As valve 7 moves downward, pm .18 which is engaged with the forked arm 30 of crank 31 pivoted at 32,.

shaft'27. and pawl 17 being then also re turned to their original positions by their respective springs.

In order to time the motion oli valve at and also to prevent it from striking a blow on its respective seats, I provide an additional arm 37 rigidly attached to it so that when.

the valve moves it operates a piston 38 in an oil dash pot 39 or other equivalent device. By an arrangement of suitable grooves and by-passes in the dash pot cylinder the motion of valve 1 maybe completely controlled in any desired manner, thus for instance it may be made to pause before coming against either of its seats.

Although a single valve 4: afiords the simplest construction, two ordinary non-return valves suitably linked together, one controlling the supply pipe and the other the g ischgrge pipe, may be used as shown in When the head or pressure of the liquid in the supply tankis such that the liquid flowing into the chamber to; expel the products would over-run the level of'the exhaust valve, the oscillation necessary for theintake of a fresh charge may be obtained in a manner which will be explainedwith reference to Fig. 10. The supply tank 58 is here shown at a higher level than the top of the chamber- 1, a a being the level of the liquid in the tank. Assuming that a compressed charge exists above the level bb lio Liquid flowing from the supply tank rises I in the combustion chamber and expels the products of combustion, but as the level of llqllld '1n the supply tank is such that the liquid in the combustion chamber tends to rise above the level of the valve 6, this valve may be shut by the impact of the rising liquid, and the further motion of the liquid arrested by the cushioning of the exhaust products entrapped in the top of the com-- bustion chamber above the level of the valve 6. This cushioning puts the entrapped products under pressure to an extent depending principally upon the velocity of flow when the valve 6 shuts, and the elasticcushionex anding, drives down the liquid in the com ustion chamber so that after its level arrives at that of valve 6 its furthermotion draws in a fresh combustible charge ast the inlet valve 7. The level of the iquid having reached its lowest point, some sion is produced by an inwardly flowing column of liquid in the discharge pipe as already described.

A. suitable valve gear for the cycle last described is shown in Fig. 2, and in Fig. 5 drawn to an enlarged scale. .The exhaust valve 6 is normally held up by a pawl engaging under a collar 41 fixed on the valve stem, but even when pawl 40 is disengaged, the valve 6 continues to be held up by a small roller42 pressed against the inclined surface d3 of a suitably shaped part attached to the stem of the valve, by a-spring 4:4 acting' on the lever 45 pivoted at 4:6. The weight of the exhaust valve 6 with its stem and fittings may be so adjusted that the valve opens when the pressure inside the chamber is somewhat less than the outside pressure. This occurs at the end of the expansion stroke, at which time, as will presently be seen, pawl l() is clear of collar 41. Valve 6 in opening has to press out the roller 42 and lurther, by means oi. pin l? which engages crank l8 operates through link 49 crank 50, bringing the arm 51 of this crank against a pin 52 on the stem of valve 7. This position is rendered stable owing to the shifting of spring 53 to the other side of the pivot 54. The movement just described puts tension upon spring 55 and relieves the tension on spring 56 both of which are attached tothe link 57 and to the respective cranks as shown. The effect is that pawl 40 and pawl 1? are both urged toward the left, but are prevented from moving in that direction by the collar all until exhaust valve rises and permits pawl 40 to engage under the said collar, thus holding'up the exhaust valve and releasing the inlet valve 'i'. l-litter the exhaust valve has opened it remains open until shut by impact of the liquid upon it as already described. immediately valve 6 comes on its seat the pawl 40 engages under the collar 41 and pawl. 17 is moved clear of collar 16 on inlet valve 7. Thus, after thecushioning stroke has occurred the inlet valve 7 is tree to open and admit a fresh combustible charge. This valve closes again under the action or spring 15. When the inlet valve opens, pin 52 on its stem, en aging with the end of crank 51, returns this crank to its first position where it is then held by the spring 53 which is now on the right of the pivot 54. 7 Further, tension is put on spring 56 and relieved in spring 55 so that when the inlet valve shuts, pawl 17 again engages under the collar 16 and pawl 10 is moved clear of the collar 41 on the exhaust valve. In this position the cycle'is ready to be re-started In Fig. 3 an alternative arrangement for the valve 4 is'shown. Instead of apivoted -valve with two faces, there are two mushroom valves rigidly connected so as to form in reality one valve with two seats. It performs the same functions as the pivoted valve. However constructed, valve 4 may be controlled as already stated.- Thus, for instance, in the cycle last considered, the valve 4 may be made to move slowly from the position in which it closes communication between the supply pipe and the combustion chamber and thus permits the pressure in the combustion chamber to reach atmospheric pressure or thereabouts in spite of the head of water in the supply tank tending to open wide the valve d before this pressure is arrived at. 1

The precise action of the apparatus may be varied by simply altering the arrangement of the connections between the combustion chamber and the liquid supply and delivery pipes respectively, and the arrangement of the auxiliary suction pipe and its connections with the supply pipe, it there be such connections, and the delivery pipe.

As an illustration or this, Flg. 6 shows in full lines a short connection 2-2, between the supply tank 58 and the combustion chamber with a separate connection of the tank with the auxiliary suction pipe 20, this connection being fitted with a cook 59 and a non-return valve 9. The drawing further shows the discharge pipe arranged with. a nozzle 60 in an annular space 61 so that the liquid issuing from the nozzle may have an injector action upon the surrounding 11(1- uid and cause liquid to How through. the auxiliary suction pipe as it it were flowing under a greater head than the actual head.

In Fig. 7 is shown a long supply pipe connecting the supply tank with the combustion chamber so as to give greater inertia to the column oi? liquid moving in this pipe, the efl'ect of which is to lengthen the time of oscillation of the liquid and so prolong the period of exhaust and admission.

The auxiliary suction pipe may be connected with the long su ply pipe instead of being connected directy with the supply tank,

For modifying the re uired oscillation by and inductive action of die liquid set in motion by the combustion I provide an ar rangement such as is shown in Fig. 7. Here the inlet 2O of the auxiliary suction pipe is so placed in relation to the supply pipe that liquid flowing in the former will have an inductive action on liquid flowing in the latter. i

Instead suction pipe of Fig. 6 I provide a throttle valve 62 or its equivalent, as shown in Fig.

as the valve 4: begins to change its position and before a free passage for the liquid is opened through the auxiliary suction pipe. The effect is increased if the movement of valve lis retarded. so as'to give time for v some of the liquid in the supply pipe to pass over the valve a and into the discharge pipe before valve 62 opens.

In Fig. 8is shown, in diagrammatic form, some of the possible arrangements of the supply tanks in relation to the apparatus itself. Thus the auxiliary supply pipe may be connected either to a separate low level tank below the level of the discharge pipe 3, or to a separate tank above the level of the discharge pipe. g

It is sometimes preferable to insure that the combustible charge taken in shall be a definite one, in which case the apparatus may be provided with a measuring device introduced either into the supply pipe or into the discharge pipe. Fig. 11 illustrates one of several forms which such a device may take. In thesupply pipe 2 is a piston valve 65 attached to a rod' 66 and capable of move ing into the dotted position 65 in which liquid can flow past the piston into the combustion chamber to expel the products of combustion. As soon, however, as this liquid begins to return toward the supply tank and to drawv in a fresh combustible charge, the iston enters into the cylindrical portion of t .e supply pipe in which it forms a freely moving piston, and thus, by its limited motion in passing from the position to the position 65 measures into the cylinder a more or less definite quantity of combustible charge. There may be in the discharge ipe a throttle valve or the like 67 actuated by arm 68 attached by link 69 to an arm '69 pivoted to a projection on the wall of the combustion chamber.

curs the throttle valve is open an the piston proceeds b its further motion to shut the throttle va ve. The throttle valve remains shut and so prevents any liquid return ng along the discharge pipe into the combust on of the cock shown in the auxiliary,

When ex losion 00- inseam chamber until the piston valve returning to its seat causes a tappet 70 on the piston rod to engage arm 69 andfso open the throttle valve 67. The liquid column in the discharge pipe is now free toreturn and compress the combustible charge which has been drawn in.

It is not essential that the fresh charge or the whole thereof or both constituents thereof, should be drawn in at the top of the combustion chamber; when desirable there may be substituted for the inlet valve 7, or this valve may be supplimented by, another valve situated in the delivery pipe as shown at 71 in Fig. 12. When valve 4 swings into position 4* as already described, the liquid in pipe 3 is moving with considerable velocity "and draws in a charge through thevialve 71'. The degree of suction produced in the regions of this valve depends, among other things, upon the degree of freedom with which liquid can be drawn. through the auxiliary suction pipe 20 past the valve 9 to follow the moving liquid in the discharge pipe. Consequently thereof, at each cycle,'there may be an at.

tachment consisting mainly of two valves 72 and 7 3 controlling respectively a pipe 7 5 which admits the combustible mixture or a constituent-thereof, and a pipe 7 6 dipping into liquid at say the level 6 e. The action 71 opens, and the combustible charge, or a constituent thereof, is drawn in. But valve 71 is connected with valve 72 by the link 7 so that when valve 71 opens, valve 72 is closed. The suction draws liquid up the pipe 7 6 from the level e e to the level f f thus displacing combustible charge by llquid until the liquid shuts valve 73. As the volume of liquid between the two levels is a definite amount, this arrangement permits a given mixture drawn in through pipe 75 past valve-72 whenthe valve 71 is shut and the liquid in pipe 7 6 tends to return to its normal level, can be varied. This device, which in eiiect consists of a liquid piston moving between difinite limits, may also be applied to the inlet valve 7.

If the whole of the constituents of the combustible mixture are drawn'in through valve 71 it is desirablethat the height of th liquid in the main supply tank should,

be such that, when the liquid flows from the supply pipe into the combustion. chamber,

. ofthis part of the apparatus is as follows:- When valve 4 comes into pos1t1on 4 valve 7 valve 4and so direct it should just rise to the height required to drive out the products of combustion, also the liquid should not be allowed to return. In this case a non-return valve 78 is fitted in the supply pipe so that when the liquid rises in the combustion chamber by its momentum above the level of the liquid in the supply tank it may be maintained at its level and no reverse flow may occur. As the exhaust valve may conveniently open when valve 4 moves to position 4 and close when valve 4 has returned, the exhaust valve may be directly operated by valve 4 through arm 79, rod 80, and lever 81. The cycle of operations for the apparatus as a whole need not be repeated, but it should be stated that after the outwardly moving column of liquid in the discharge pipe has come to rest the combustible charge of constituent which has been drawn into the sloping portion of the discharge pipe is swept by the inwardly moving column of liquid into the combustion chamber, and therein compressed. When only ione constituent of the combustible mixture or a portion of the combustible mixture is drawn in at valve 71 the non-return valve 78 may be dispensed with, and the other constituent or the other portion of the combustible mixture may be drawn in in the usual manner through valve 7.

A somewhat modified working of the apparatus is obtained it there be no valve clOS- ing the communication between the chamber 1 and the discharge pipe. Such a n1odification is shown in Fig. 13, in u hich the motion otvalve 4 is limited by means of the stop 82. In this case the auxiliary suction pipe may be dispensed with because when valve 4 opens the communication with the supply pipe in the usual manner, toward the end of the expansion stroke liquid can flow from the supply ipe 2 over the top of y into the discharge pipe 3, as well as into the combustion chamher in which the liquid rises to ex el the burnt products and falls again to raw in a fresh charge in the manner already described, and when this has hap ened the returnin column of liquid in t e dischar e pipe c oses valve 4 and com resses t e charge. If valve 4 is controlle by a dash pot or equivalent arrangement, so that it toes not close immediately on the return of the column of liquid in the discharge pipe, some of this li ui may flow in the reverse direction over t e top of the valve and into the supply pipe, thus allowing'the velocity of the returning column of liquid to increase beyond that'which it would otherwise have attained when valve 4 shuts, The additional kinetic energy stored in the moving column of liquid will then give rise to a hi her comression ressure of the combustib e charge. his met 0d of increasing the compression it liquid-from the supply applies in general and is not confined to this particular case. In this, as in other cases, expansion may be continued beyond atmospheric pressure without loss of energy, because, if the exhaust and inlet valves are kept closed long enough, work will be done by the external atmosphere in forcing liquid into the combustion chamber until atmospheric pressure is again attained.

Where the exhaust and inlet valves are sucked open, and in opening these valves have to move valve gear requiring the expenditure of a small amount of power, the valves themselves may, for a portion of their travel, act as pistons in a prolongation of their valve seats, as shown in Figs. 4 andv 5.

Another simple method of introducing the combustible charge in this case explained in connection with the form of apparatus shown in Fig. 13, may now be described in connection with Fig. 24. Between the liquid in the supply tank 58 and the supply pipe 2 is placed a bell 168 or other chamber with 'means of restricting the flow of liquid between the tank and the supply pipe; such, for instance, as a number of holes 169 perforated in the bell, the amount of opening of which an be regulated by a perforated band 170, the holes in which can be made to register more or less with the holes in the bell. The bell has at its upper part one or more inlets 171, 172 for the introduction of the constituents of the combustible charge. When valve 4 is in that position that it closes communication between the combustion chamber and the supply pipe, the liquid in the tank tends to level itself and rise to the same level in the bell through the holes. Toward the end of the expansion stroke, when valve 4 takes up its dotted posit1 on, liquid from the bell enters the combustion chamber and expels products of combustion.

If the exhaust valve is shut, and the inlet valve is not allowed to open, or only opens under a sufliciently stilt spring, the liquid flowin in the discharge pipe will draw after pipe in the manner already. described. Should this demand for liquid be greater than the total supply through the holes in the bell, air or combustible, or both, will be drawn through the ipes 171, 17 2, into the supply pipe and comustion chamber, until the charge pipe having come to rest, a column of liquid starts to flow inwardly, closes valve 4, and compresses the combustible charge in the combustion chamber. While this valve is closed, so much of the combustible charge as was in the supply ipe and lower portion of the bell is rep aced by liquid from the supply-tank flowing through the holes in the bell, and when the liquid level in the bell has risen sufliciently, everything is ready for starting a fresh cycle.

The application of air vessels will now be liquid in the dis explained with reference to Figs. 14:, 16

pressures, or, in other words, by the dimensions of the pipes in which these columns move. It would be inconvenient to alter the dimensions of the pipes for the purpose of varying the periodicity of the cycle but the desired effect may be obtained by the use of air vessels, intensifiersor accumulators communicating with the said pipes. -It will be suficient to explain the efi'ect of introducing air vessels, intensifiers, or accumulators into the discharge pipe or conduit as shown in Fig. 14. These air vessels may be controlled by cocks, and when these cocks are shut the full length of the discharge pipe is effective as regards the resulting periodicity. In the cock 83 on air vessel 84: is opened, liquid forced from the combustion chamber during the working stroke causes liquid from the discharge pipe to enter.

the air vessel, but on the return stroke, when the liquid flows back toward the combustion or pump chamber to compress the combustible charge, liquid leaves the air vessel again. The result is to make the efl'ective length of the discharge pipe shorter, and if the air vessel, intensifier, or accumulator 84 might be considered indefinitely large the effective length of the discharge pipe may be'considered as that between the combustion chamber and the air vessel, intensifier, or accumulator, and the flow of liquid in the discharge pipe beyond the air vessel would be more nearly continuous. The effect of the air vessel depends on its capacity, and as it would involve a loss of energy to throttle the liquid inlet by means of the cock 83 it is better to add an additional air vessel 85 the communication with which can be controlled. by the cock 86. It will be noticed that: when air vessels are used in the manner described they accumulate or store up energy in an elastic cushion 1 during the working stroke'and give out en again during the compression stroke.

en an air vessel 87 is used 1n the discharge pipe, with the object of producing a continuous flow, such air vessel maybe fitted with a non-return inlet valve, as shown in Fig. 16, and in this case a second air vessel may be used to store the-energy for compression of they combustible-charge by thereturning mass of liquid in the manner already described. Such second air vessel is shown at 88 as fitted with a'valve 89 attached to a float, so that when the liquid has risen to a given height thefloat closes the valve. In operatiom'jthe column of liq- ;uid flowing outward from the combustion assume chamber flows first into air vessel 88 until thelevel of liquid therein attains a height at which the float closes the valve and this should be so adjusted that the available ens ergy then stored in the elastic cushion'rep resents that required for giving the com: pression stroke. When valve 89 closes, the column of liquid in the discharge pipe has a considerable velocity and as its motion cannot be instantly arrested by the closing of valve 89 the flow continues, and valve 90 on airvessel 87 is forced open and liquid flows into air vessel 87 until the energy of motion is. expended. This arrangement of air vessels is preferred in the case where I use the liquid to drive a Pelton wheel as before mentioned, because it is desirable to use a higher pressure in that case than is required for other impulse or reaction-turbines, and the arrangement permits of much higher pressures being attained, as the pressure in air vessel 87 may exceed any of the working pressures in the combustionchamber. The valve on air vessel 88 may be controlled so as to shut when the elastic cushion in the air vessel has a predetermined pressure, and for this purpose any suitable means may be used to close the valve when the pressure of the elastic cushion overcomes an opposing -pres-, sure and so gives motion to the valve. In

the case where even higher liquid pressures are required and to still obtain complete expansion of the products in the combustion chamber, there may be another valve 91 at the end of the discharge pipe which is kept normally open by a spring and is closed.

when the liquid flowing past it reaches a given velocity on the principle of the Well known hydraulic ram. In thiscase liquid flowing in the discharge pipe first runs to waste through valve 91 while the velocity of flow in the discharge pipe is increasing, then valve, 91 suddenly shuts, causing the liquid to flow first into air vessel 88 and then into air vessel 87 in the manner already explained. Fig. 17 shows a similar arrangement to that last described, but without any valve or float in air vessel 88. Consequently the elastic cushion pressure in theair vessel 88 must become equal to the pressure inthe air vessel '87 before valve opens, and in this case, owing to the higher pressure, the quantity of elastic fluid in air vessel 88, re-

uired to store the ener for compressing t e combustible charge wi 1 be less than if a larger volume of elastic fluid is used and the pressure kept lower as in the arrange ment of Fig. 16.

As already stated, the delivery and suction pipes may be duplicated and so arranged that thevforces developed tend to balance, each other.

A duplication of the discharge pipe may also serve to make the apparatus operate may branch into. two ipes 3 and 3. If each of these ipes is 0 the same length and diameter as t e one discharge pipe which they replace, the time of the cycle will be shortened. If the branch 3 is longer than the branch 3 and non-return valves 92 and 93 are introduced as shown, so that the branch 3 becomes the passage for the outwardly flowing liquid and 3 the passage for the return flow, then a more continuous flow can be obtained in the branch 3, and such 1 an arrangement is shown in Fig. 15. When valve 4 moves to its position 4 both valves 9 and 92 will open to suppl liquid to follow the moving liquid in the discharge pi e 3, but by proper adjustment liquid wi 1 be mostly drawn through the short connection at 20 because of the greater inertia of the liquid in the return pipe 3 which has to be started from rest. After valve 9 shuts, liquid from the return pipe will flow into the combustion chamber, givin the compression stroke, but some liquid roin the return pipe may also continueto follow the liquid moving in the discharge pipe, so that the direction of flow inthe discharge pipe may, under some circumstances, never be reversed. When the ressure rises on combustion, valve 92 shuts. ipes 3 and 3* may lead to separate reservoirs at different levels.

Where it is not convenient to place the is under pressure during the working stroke a portion of the liquid may flow past valve 96 into the air vessel 94: and so compress the elastic cushion and store energy. The energy thus stored may be-released when valve 4 changes its position, and for this purpose the .valve 4: may be connected b an arm 97, a link 98, and another arm 99 with a throttle valve 100 or its equivalent. When the throttle valve 100 is opened the elastic cushion in the air vessel 94 expands and drives liquid through pipe 101 in such manner that it has the action of an injector and raises water from the supply tank into the combustion chamber. The amount of the charge drawn in, being determined by the quantity of liquid which flows back to the supply tank, may be regulated by means of a non-return valve 102 and a control by-pass 103.

Another means of lifting liquid from a low'level su ply tank is shown in Fi 19, the chief di erence from the last case being that the portion of the energy at each cycle which is utilized for raising the liquid is di- 105 and to compress an elastic cushion in the top portion of this cylinder. Thus, either high pressure liquid or high pressure products of combustion may be conducted to the charge of the operating medium. Piston 104 is attached by rod 109 to piston 110 working in cylinder 111, and on the upward stroke the liquid is drawn into the cylinder through valve 112 and on the down stroke is discharged through valve 113, the discharged liquid being arran ed to have an injector action and so raise iquid from the low level supply tank in the manner previously described. The release of the elastic cushion may be brought about by the action of valve 4: through arm 97, rod 98 and crank 114 as shown.

In the foregoing description the combustible charge has been drawn into the apparatus. The charge may equall well beintroduced under pressure and or this purpose it may be pumped in or otherwise forced in by any known device preferably after the products of combustion have been expelled. It is economical, however, to apply a portion of the energy of the combustion at each cycle to put the combustible mixture or a constituent thereof under sufiicient pressure to enable it to enter the chamber at the desired moment.

Thus in Fig. 20 a separate air vessel 115 is connected with the combustion chamber 1 or to the discharge pipe at such level that the connection is always below the level of the liquid. A portion of the energy of combustion at each cycle compresses air in this vessel and stores it in a carburetor 116 so that when the stored air is released by the opening of the throttle valve 120 by the downward movement of the inlet valve 7 operating, through crank 117, link 118, and arm 119, the compressed air flowing through pipe 121 may draw with it petrol or other combustible liquid through the small pipe 122 and inject it in an atomized condition, along with the air supply, through pipe 121. An air inlet valve 123 is fitted to the air vessel 115, and a non-return valve 124.. It should be observed that pressures exceeding the explosion pressure mag be obtained in the air vessel 115 owing to t e momentum of the intervening column of liquid and the relatively smaller size of the air vessel 115 as compared with the combustion chamber 1.

Another device for the same purpose is shown in Fig. 22. A number of pistons, 127, 128, 129, in this case limited to three, are linked together by a rod 130. One of the pistons, 128, is adapted to beacted upon either by the fluid which is subject to the pressure of the ignited combustible gases or directly by the ignited gases themselves,

and the said piston is preferably placed in v a branch or limb 138 of the discharge pipe or of the combustion chamber- In the present case the piston is shown as acted 'u 'on by thefluid in the dischar e pipe. he

piston 127 works in a cylin er 131 in the" upper part of which is fitted an inlet valve 141 for combustible charge and an outlet valve 143 controlling a pipe 132 which leads purpose the piston 129 may work in a dash previously drawn in by an oscillation in the pot 135 fitted with a by-pass136 controlled by an equilibrium or other valve 137. The branch 138 in which piston 128 works is prolonged and turned upward with a closed end so as to form the air vessel 139. The piston 128 will then work with liquid on both sides, and the air vessel 139 will serve to store energy in the same manner as the elastic cushion in the lower portion 133 of cylinder 131. When combustion occurs in chamber 1 the piston 128 makesa downward stroke, which is limited by the pressure of the elastic cushion, and is locked in position by the oil or other fluid in the dash pot 135 whichpasses freely through valves 140 from the bottom to the top side of the piston 129 during the downward stroke, but is unable to return. During the.

said downward stroke combustible charge,

or a constituent thereof, is drawn in through c the valve 141 which may close under the action of a spring. When valve- 4, having changed its position, returns to its first po sition and so closes communicationbetween 133, and of the air vessel 139. The linked plstons then make an; upward stroke, and

the combustible charge drawn into the to part of cylinder 131, or a portion thereo 1s forced past valve 143 and valve 7 into the combustion chamber. When thisoccurs there may, if desired,.already be in the top portion of the combustion chamber a quantlty of air or other combustible constituent chamber of the kindalready described. For

a given pressure of combustion'the quantity of combustible charge drawn into the cylinder 131 will depend on the original volume and pressure of the elastic cushioning.

medium contained in the portion 133 of the cylinder if air vessel 139 is not used, consequently the length of stroke maybe altered by varying the effective volume. For the latter purpose an additional air vessel 145 communicating with the lower p0rtion'133 of cylinder 131 and controlled by-a cock 134 may be used. Thus when this cock is open, the eflective quantity of elastic medium is that contained both in the lower portion 133 of cylinder 131 and in the air vessel 145. By varying the amount of opening of cock 134 the quantity of charge drawn in, and subsequently forced into the Again, by varying the relative diameters of the pistons 127 and 128 the pressure at which the combustible charge is forced into the combustion chamber may be varied,

When it is desirable that the liquid in the combustion chamber which comes into contact with the burnt gases, and may be at 174, 175, the diaphragm being clamped in a suitable enlargement of the dlschargepipe 3 as shown. he volumeinclosed betweenthe two extremepositions of the diaphragm must be suflicient to accommodate the amount of liquid which leaves the combustion chamber during the combustion and expansion, stroke, and valve 4 must not be allowed to close communication between the supply pipe 2 and the combustion chamber 1 on the return stroke of the liquid in the discharge pipe until that quantity of liquid or thereabout, which entered the combustion chamber from the supply pipe, has been allowed to return thereto. To accomplish this end there are fitted in the diaphragm These arms are connected by rods 183 and 184 to a bell crank 185 and again through chamber 176 two' buffers 177 and 178 working on spindles 179 andv180 which pass through glands and are connected out- .side the chamber to arms 181 and 182.

combustion chamber, can be regulated.

link 186 to another arm 187 so as to operate the by-pass valves 188 and 189 in the dash pot 39 which controls the'motion of valve 4.

If on the working stroke so much liquid passes from the combustion chamber into the diaphragm chamber as would tend to force the diaphragm too far to the right, bufier 178 is turned about spindle 180 and bypass valve 188 is opened to a greater extent, and the other by-pass valve 189 is shut to a greater extent. Thus the dash-pot piston 38 has a less resistance in moving from the position shown by full lines to the position shown by dotted lines, and a greater resistance in passing back to the former position. Consequently valve 4 moves more quickly from the full line position to the dotted line position 1", and more slowly from the dotted line position to the full line position, and more liquid isallowed to return from the combustion chamber into the sup ply pipe before valve 1 closes. On the next stroke, therefore, there will be less liquid between the full line position of valve 4 and the diaphragm, so the diaphragm will not be distended so far to the right. On the other hand, if the diaphragm tends to be distended too much to the left the action upon the by-passvalves 188, 189 is the opposite to that last described, as they are then turned by the motion of buifer 177 in the opposite direction, resulting in a greater resistance to the movement of valve 4 from the full line position to the dotted line position, and a less resistance to its motion in the opposite direction. Consequently valve 4 shuts in its full line position earlier than before, and more liquid is retained between the full line position of valve 4: and the diaphragm, so that on the next working stroke the diaphragm moves rather farther to the'right. It will be seen that by the automatic arrangement the quantity of liquid which enters and leaves the combustion chamber remains practically unaltered and is entirely separated from the liquid in the discharge pipe or the liquid which enters past the auxiliary supply valve 9.

Instead of using a diaphragm, as in the case last mentioned, the liquid which enters and leaves the combustion chamber may be isolated from the liquid which flows in and is delivered from the discharge pipe by means of a liquid metallic piston, for example a U pipe containing liquid of a reator specific ravity than the working liquid. Fig. 26 S1OWS such an arrangement where the discharge pipe 3 is bent into a. vertical U shape and contains a dense fluid such as mercury, in the bottom of the U, as

shown at n n. On the working stroke, when liquid is propelled along the discharge pifae, the dense liquid is depressed in limb 90 and elevated in limb 191, and when the liquid returns in the discharge pipe the dense liquid is depressed in limb 191 and elevated in limb 190. In order to prevent the dense liquid from being driven too far toward the discharge pipe Or combustion chamber respectively, floats 192, 193, of such" weight as to be acted upon only by the dense fluid when it rises to their level, may be placed in the two limbs of the U pipe. The lifting of either of these floats operates the by-pass valves 188, 189, and so controls the other words, the dense liquid takes the place of the diaphragm, and the floats take the place of the bulfers.

So far, only one connection has been shown for conveyingliquid to or from the combustion chamber 1 and the supply tank, although the multiplication of connections has been mentioned. It is obvious that the action of the apparatus is not materially altered by such multiplication of pipes, and that the pipes can be introduced at any suitable level in the combustion chamber. In Fig. 21 is shown an additional connection 125 to the combustion chamber 1 and fitted with'a valve 126. When such additional pipe is introduced a little below the level corresponding with the maximum charge column and when the valve 126 is held open by a spring, this valve may shut by the action of the velocity of the liquid which flows past it when the return flow occurs from the discharge pipe to compress the charge. It has previously been described how the movement of valve 4 may be controlled to increase the compression pressure, and when valve 126 is used for the same purpose it has the additional advantage of lessening the shock on shutting.

The special ignition hereinbefore mentioned is shown in Fig. 23, but the chamber containing the diaphragm which merely serves to separate liquid entering and leaving the combustion chamber from the liquid which must be kept clean and enters and leaves the ignition apparatus, is not shown. A closed vessel 147 containing an elastic cushion in the upper part thereof and a body of liquid in the lower part thereof, is connected by a pipe 148 with the diaphragm chamber and is thus under the influence of the liquid in the combustion chamber. While the liquid in the latter is subject to an i11- creasing pressure, liquid will be forced through 148 past the valve 149 into the ves- Sol 147 and will thus compress the elastic medium in the .top portion of the vessel. The valve 149 can slide on rod 150 and is held in position between two springs 151, 152 which press against two stops 153, 154 and so tend to hold the valve centrally between them. Connected with the valve rod 150 is a forked extension 155 which is spanned by a cross bar 156 attached to a float 157 placed in a cup 158 containing meroury. The mercury floats the moving parts so that they move with little friction. At-

tached to the float 157 isthe conductor 159 is filled into the ill tube 165 so that at a low U tube 165 containing mercury. Into the open end of the U tube 165 another wire 166 projects. The action of the apparatus is as follows While liquid is flowing into the vessel 1&7, due to an increase of pressure in the combustion chamber, the rod 150, float 157 and brush 160 are all lifted by the infiowing' liquid, which has to escape between the in+ ternal flange 167 and the valve 149. in this. position the brush 160 does not make contact with the conductor 163. When the conpression stroke in the combustion chamber is completed and the maximum compression pressure is attained, there is a tendency. for the pressure to fall again. The compressed elastic medium inthe top of vessel 147 immediately tries to expand and thus force back liquid from vessel 147 into the diaphragm chamber. A very small reversal of flow past the valve 149 causes the valve totake up the dotted position by passing through the constricted portion or hole caused by the flange'167. This downward movementot thevalve draws down the float in the mercury cup and causes brush 160 to come in contact with the conductor 163, thus closing the ignition circuit and causing aspark or sparks.

pressure, say that of the atmosphere, the levels in the two limbs of the U tube are as shown at g g, 72 it. In this positionthe wire 164 does not dip into the mecury and the circuit cannot be completed. ll hen the pressure increases the air or other elastic medium contained in the sealed end of the U tube 165, above the mercury level, is compressed, and at any levels between a i and 7c is both wires are in contact with the mercury in the it tube. This range of levels corre sponds with the range of compression pressures, and at any pressure in this range the brush 160 coming in contact with conductor 163 can complete the iginition circuit and cause a spark. At higher pressures indicated by mercury levels above i z the mercury in the U tube is in contact with wire 164 but not with wire 166 and so the circuit cannot be completed. It will be observed that the pressure inside and outside the glass it tube is always approximately the same and the tube is therefore not subject to rupture.

The possible methodsof control of the various forms of apparatus described in this specification are very numerous. Some have already been referred to, and others may be mentioned. For instance the height or the liquid in the suction tank may be varied,

audit the liquid raised or forced is to be returned to the pump for use over again,

. aeaero I there may be two supply tanks, one overfiowin into the other, and so arranged that the height of liquid in that tank which connects with the suction pipe may be varied. The known methods for varying the work done per stroke. in ordinary gas engines may be applied to the present pump. Thus, the quantity of combustiblemixture drawn into the combustion chamber may be varied by throttling the mixture, or the quantity of gas or petrol or other combustible conthis pressure is less than the normal com- 1 pression pressure the charge may be made rather larger than usual. Such charge can be ignited by a short circuiting switch, which is at once thrown out of use again, and the rest of the operation is automatic.

it is possible that, in starting the apparatus to work, the correct proportion between the constituents of the combustible mixture may not be readily obtained and the charge may consequently be incapable of ignition, also changes in the composition may occur during running, with a like result. 111 order to cause the apparatus to continue working in spite of a misfire, the liquid inlet valve such as valve 9 in Fig. 2 may be normally held off its seat by a spring, such as is shown for controlling valve 91 of Fig. 16 or the like in such manner that during the inward flow of a. column of liquid which returns toward thev combustion chamber to compress the combustible charge liquid is allowed to flow to waste through the said valveuntil the valve is 'closed under the action of the velocity of the returning column. The column thus gains a higher velocity, than it it onlyreturned to compress the charge, and ii? the said charge is not ressure than usual, expand again much as ignited it will, after compression to a higher if there had been'a :Eeeble explosion. Valve 1 will change to the position e and the unburnt charge will be exhausted and a new charge drawn in in the usual manner, the cycle being repeated at the expense of the energy of the hi h level or presure reservoir which supplied the liquid for the returning column. As soon as a charge ignites the tension on the spring of valve 9 which held it from its seat may, if desired, be re- 7 loaded and the valve thereafter allowed to act in the normal manner as already deto the position shown in full lines it is arrested in the position which allows the discharge and the supply pipe to remain in communication long enough for some of the liquid which flows inwardly toward the combustion chamber to pass over the top of valve linto the supply pipe, thus gaining an increased velocity so that the liquid which rises in the combustion chamber to compress the fresh charge may compress it under such conditions that it expands again to a pressure low enough to bring about the movement of valve l and of the exhaust valve as in the ordinary working cycle so that the unburnt charge is swept out and a new charge introduced.

It has already been mentioned that the reservoir into which the liquid is raised or forced may be a closed reservoir, so that the upper portion thereof operates as an air vessel. It is obvious that the same idea can be applied to the supply tank, and throughout the specification the words head and pressure are generally interchangeable.

Air vessels may be used wherever required to prevent shock.

What I claim is 1. The combination of a power chamber for an elastic prime medium having pressure and expansive force, a play pipe 'for the reciprocation of a liquid column, means for communicating an actuating force from the power chamber to the liquid column, and means .for restraining said actuating force after the liquid column has been set in motion.

2. The combination of a power chamber for an elastic prime medium having pressure and expansive force, a play pipe for the reciprocation of a liquid column, means force after the liquid columnhas been set in motion.

4. The combination of a power chamber for an elastic prime medium having pressure and expansive force, a play pipe 'for the reciprocation of a liquid column, means comprising a diaphragm piston for com' municating an actuating force from the power chamber to the liquid column, and means for restraining said actuating force after the liquid column has been set in mo tion.

The combination of a power chamber for an elastic prime medium having pressure and expansive force, a play pipe for the reciprocation of a liquid column, an actuator for communicating an actuating force from the power chamber to the liquid column, and means for restraining said actuating force after the liquid column has been set in motion.

(5. The combination of a power chamber for an elastic prime medium having pressure and expansive force, a play pipe for the reciprocation of a liquid column, an actuator for communicating an actuating force from the power chamber to the liquid column, said actuator having a limited movement whereby, after the actuator comes to rest, the continued movement of the liquid column, due to its momentum, will cause the intake of fresh liquid.

7. The combination of a power chamber for an elastic prime medium having pressure and expansive force, a play pipe for the reciprocation of a liquid column, a piston in the power chamber, an actuator in operative relationship with the piston for actuating the liquid column.

8. The combination of a power chamber for an elastic prime medium having pressure and expansive force, a play pipe for the reciprocation of a liquid column, a piston in the power chamber, an actuator for actuating the liquid column, means for establishing operative relationship between piston and the actuator, and means for limiting the movement of the actuator.

9. The combination of a play pipe for the reciprocation of a liquid column with a velocity suiliciently limited to preserve the coherence of the column and having sufficient bulk and path of travel in order to acquire useful momentum, a power cylinder for an elastic prime medium having pressure and expansive force, and a piston operating therein.

10. The combination of a play pipe for the reciprocation of a liquid column with a velocity sufliciently limited to preserve the coherence of the column and having suiiicient bulk and path of travel in order to acquire useful momentum, a power cylinder for an elastic prime medium having pressure and expansive force, a piston operating therein and an accumulator connected with the play pipe for storing energy during one movement of reciprocation and for giving out energy in connection with a return stroke.

11. The combination of a play pipe for the reciprocation of a li uid column with a velocity sufiiciently limited to preserve the coherence of the column and having suiiicient bulk and path of travel in order to acquire useful momentum, a power cylinder for an elastic prime medium having pressure and expansive force, a.piston operating therein and an accumulator connected with the play pipe for storing energy during a power stroke and for giving out energy to cause a compression stroke.

12. The combination of a play pipe tor the reciprocation of a liquid column with a velocity sufficientlylimited to preserve the coherence oi the column and having suflicient bulk and path of travel in order to acquire useful momentum, a power cylinder for an elastic prime medium having pressure and expansive force and a piston operating there in the play pipe provided with liquid intalre and liquid discharge.

13. llhe. combination of a play pipe for the reciprocation of a liquid column with a velocity sufliciently limited to preserve the coherence of the column and having sufficient bulk and path of travel in order to acquire useful momentum, a power cylinder for an elastic prime medium having pressure and expansive force, and a piston operating.

therein, the play pipe provided with liquid. intake and liquid discharge, an accumulator connected with the discharge and an ad-.

'ditional accumulator connected with the play pipe to cause the return stroke of the liquid column.

14. The combination of a play pipe for the reciprocation of a liquid column, a power chamber connected with said play pipe for a pr1mary medium having initial pressure and subsequent expansive force, said chamber provided with an admission valve and an exhaust valve, the exhaust valve arranged to be shut by the impact upon it of liquid flowing into said chamber.

15. The combination of a lay pipe for the reciprocation of a liquid co umn, a power chamber connected with said play pipe for a primary medium having initial pressure and subsequent expansive force, said cham-f ber provided with an admission valve and an exhaust valve,-and a valve gear adapted to retard the opening of the exhaust valve and to permit it to be shut by the impact upon it w of liquid flowing into said chamber.

16. The combination of a play pipe for the reciprocation of a liquid column, a power chamber connected. with said play pipe for a subsequent expansive force, said chamber,

provided with an admission. valve and an exhaust valve, a mechanism for controlling said valves comprising means whereby the inlet valve opens under suction and in closing automatically releases the exhaust valve,

the exhaust valve adapted to open when the pressure within the chamber has fallen to a suitable extent and to be shut by impact of liquid upon it and in closing to release the admission valve and whereby each valve on shutting is locked as aforesaid,

WEBER? HUELPHREY.

lllitnesses:

' Josnrn J. dad-serum. 

